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High-resolution C-isotope chemostratigraphy of the uppermost Cambrian stage (Stage 10) in South China: implications for defining the base of Stage 10 and palaeoenvironmental change

Published online by Cambridge University Press:  17 April 2017

DANDAN LI
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
XIAOLIN ZHANG*
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
KEFAN CHEN
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
GUIJIE ZHANG
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
XIAOYAN CHEN
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
WEI HUANG
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
SHANCHI PENG
Affiliation:
LPS, Nanjing Institute of Geology and Palaeontology, Chinese Academy of Sciences, Nanjing 210008, China
YANAN SHEN
Affiliation:
School of Earth and Space Sciences, University of Science and Technology of China, Hefei 230026, China
*
†Author for correspondence: zhxl2012@ustc.edu.cn
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Abstract

The Wa'ergang section in South China has been proposed as a potential Global Stratotype Section and Point (GSSP) for the base of Stage 10, the uppermost stage of the Cambrian System. In this study, high-resolution C-isotopic compositions are reported and we identified three large negative δ13C excursions, namely N1, N2 and N3, at Wa'ergang. The N1 is located just above the First Appearance Datum (FAD) of Lotagnostus americanus, corresponding to the possible base of the Proconodontus posterocostatus conodont Zone. The N2 was identified within the Micragnostus chuishuensis trilobite Zone and the Proconodontus muelleri conodont Zone. The N3 is located in the lowermost part of the Leiagnostus cf. bexelli – Archaeuloma taoyuanense trilobite Zone or Eoconodontus conodont Zone. The N1 and N2 can be correlated with the negative δ13C excursions preceding the Top of Cambrian Carbon Isotope Excursion (TOCE) observed globally. The N3 can be correlated with the TOCE or the HEllnmaria–Red Tops Boundary (HERB) Event. The inter-basinal correlation of N1 and L. americanus strongly supports that the base of Stage 10 may be best defined by the FAD of L. americanus. We also used a box model to quantitatively explore the genesis of the negative δ13C excursions from South China. Our numerical simulations suggest that weathering of the organic-rich sediments on the platform, probably driven by intermittent sea level fall and/or the oxygenation of the Dissolved Organic Carbon (DOC) reservoir in seawater, may have contributed to the generation of the negative δ13C excursions observed in the Stage 10 at Wa'ergang in South China.

Information

Type
Original Articles
Copyright
Copyright © Cambridge University Press 2017 
Figure 0

Figure 1. The location of the Wa'ergang section in South China (revised from Peng et al.2014).

Figure 1

Figure 2. δ13C and δ18O stratigraphy for the Wa'ergang section in South China. Biozone data are from Peng (1990a, 1992), Peng et al. (2015) and Bagnoli et al. (2017).

Figure 2

Table 1. δ13C and δ18O of samples from the Wa'ergang section, Hunan, SW China

Figure 3

Figure 3. Cross-plot of δ18O and δ13C for the Wa'ergang section.

Figure 4

Figure 4. Global correlation of the upper Cambrian of the Wa'ergang section. Trilobite zone: L. c. – S. b. — Leiostegium constrictum – Shenjiawania brevis; M. s. – F. — Mictosaukia striata – Fatocephalus; L. b. – A. t. — Leiagnostus cf. bexelli – Archaeuloma taoyuanense; M. c. — Micragnostus chuishuensis; L. a. — Lotagnostus americanus; E. d. — Eolotagnostus decorus; M. p. — Mictosaukia perplexa; N. q. – S. n. — Neoagnostus quasibilobus – Shergoldia nomas; S. i. — Sinosaukia impages; R.c. m. — Rhaptagnostus clarki maximus; R. p. — R. papilio; R. b. – N. d. — R. bifax – N. denticulatus; R.c. pr. — R. clarki prolatus; C. s. — Caznaia sectatrix; R.c. pa. – C. sa. — R. clarki patulus – Caznaia squamosa. Conodont Zone: E. — Eoconodontus; C. m. — Cambrooistodus minutus Subzone; E. n. — Eoconodontus notchpeakensis Subzone; P. m. — Proconodontus muelleri; P. p. — Proconodontus posterocostatus; P. t. — Proconodontus tenuiserratus; C. h. — Chosonodina herfurthi; C. a. — Cordylodus angulatus; C. l. — Cordylodus lindstromi s.s.; C. pr. — Cordylodus prolindstromi; H. s. — Hirsutodontus simplex; C. p. — Cordylodus proavus.

Figure 5

Table 2. Fluxes and carbon isotope values from boundary parameters used in the model

Figure 6

Figure 5. Comparison between the δ13C record and the modelling result.

Figure 7

Figure 6. A sensitivity test for the box model where the initial mass of marine DIC was varied. All other model parameters were held constant, with the exception of the influx of oxygenation of organic carbon, which we increased 1.7-fold for 0.12 Ma to simulate the N1 and/or N2 carbon excursion (a). Similarly, we increased it 1.5-fold for 0.28 Ma to simulate the N3 carbon excursion (b). The model result indicates that decreasing ocean DIC mass increases the magnitude of the excursion and decreases duration of the isotope recovery of the DIC reservoir.